U.S. patent application number 12/138163 was filed with the patent office on 2010-08-05 for optical air data systems and methods.
This patent application is currently assigned to Ophir Corporation. Invention is credited to Phillip E. Acott, Loren M. Caldwell, Martin O'Brien, Lisa G. Spaeth, Shoou-yu Tang.
Application Number | 20100195100 12/138163 |
Document ID | / |
Family ID | 55404913 |
Filed Date | 2010-08-05 |
United States Patent
Application |
20100195100 |
Kind Code |
A9 |
Caldwell; Loren M. ; et
al. |
August 5, 2010 |
Optical Air Data Systems And Methods
Abstract
Systems and methods for sensing air includes at least one, and
in some embodiments three, transceivers for projecting the laser
energy as laser radiation to the air. The transceivers are scanned
or aligned along several different axes. Each transceiver receives
laser energy as it is backscattered from the air. A computer
processes signals from the transceivers to distinguish molecular
scattered laser radiation from aerosol scattered laser radiation
and determines air temperatures, wind speeds, and wind directions
based on the scattered laser radiation. Applications of the system
to wind power site evaluation, wind turbine control, traffic
safety, general meteorological monitoring and airport safety are
presented.
Inventors: |
Caldwell; Loren M.; (Ft.
Collins, CO) ; Tang; Shoou-yu; (Ft. Collins, CO)
; Acott; Phillip E.; (Ft. Collins, CO) ; Spaeth;
Lisa G.; (Littleton, CO) ; O'Brien; Martin;
(Conifer, CO) |
Correspondence
Address: |
LATHROP & GAGE LLP
4845 PEARL EAST CIRCLE, SUITE 201
BOULDER
CO
80301
US
|
Assignee: |
Ophir Corporation
Littleton
CO
|
Prior
Publication: |
|
Document Identifier |
Publication Date |
|
US 20090046289 A1 |
February 19, 2009 |
|
|
Family ID: |
55404913 |
Appl. No.: |
12/138163 |
Filed: |
June 12, 2008 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
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11488259 |
Jul 17, 2006 |
7564539 |
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12138163 |
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11103020 |
Apr 11, 2005 |
7400385 |
|
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11488259 |
|
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10632735 |
Aug 1, 2003 |
6894768 |
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11103020 |
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60699630 |
Jul 15, 2005 |
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60400462 |
Aug 2, 2002 |
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Current U.S.
Class: |
356/341 |
Current CPC
Class: |
F03D 17/00 20160501;
G01P 13/025 20130101; G01P 5/26 20130101; G01S 17/58 20130101; Y02E
10/723 20130101; F05B 2270/8042 20130101; G01N 2021/4709 20130101;
G01S 7/481 20130101; F03D 7/02 20130101; F05B 2270/325 20130101;
Y02E 10/72 20130101; Y02A 90/10 20180101; F05B 2270/321 20130101;
G01S 17/95 20130101; G01S 7/4811 20130101; G01S 7/4817 20130101;
F05B 2270/32 20130101; Y02A 90/19 20180101; G01S 17/88 20130101;
G01S 7/497 20130101; G01S 17/87 20130101; G01N 21/53 20130101 |
Class at
Publication: |
356/341 |
International
Class: |
G01P 3/36 20060101
G01P003/36 |
Goverment Interests
U.S. GOVERNMENT RIGHTS
[0002] This invention was made in part with the support of the U.S.
Government; the U.S. Government has certain rights in this
invention as provided for by the terms of Grant #NAS4-02043 awarded
by the NASA Dryden Flight Research Center.
Claims
1. A method for remotely sensing air, comprising: generating laser
radiation with a tunable laser; splitting the laser radiation into
a projected component and a control component; converting the
control component into one or more electronic control signals;
projecting the projected component into the air to induce scattered
radiation; receiving a portion of the scattered radiation as
backscattered radiation; converting the backscattered radiation
into one or more electronic backscattered radiation signals,
including converting the first portion to an unfiltered
backscattered electronic signal, filtering at least a portion of
the backscattered radiation using an optical notch filter to form a
filtered portion, and converting the filtered portion to a filtered
backscattered electronic signal; processing the one or more
electronic control signals and the one or more electronic
backscattered radiation signals to determine Doppler shift; and
processing the Doppler shift to determine wind speed.
2. The method of claim 1 wherein at least one electronic control
signal is derived by filtering the control component with the
optical notch filter.
3. The method of claim 2 wherein laser radiation is projected along
at least two axes, wherein Doppler shift is determined along each
of the axes, and wherein the Doppler shift along each of the axes
is used to determine wind speed and direction.
4. The method of claim 3 wherein laser radiation is projected along
at least three axes, wherein Doppler shift is determined along each
of the axes, and wherein the Doppler shift along each of the axes
is used to determine wind speed and direction.
5. The method of claim 3 further comprising determining air
temperature from a Rayleigh-scattered component of the
backscattered radiation.
6. The method of claim 4 further comprising scanning the laser
radiation to obtain windspeed and wind direction information at
multiple locations within a volume of air.
7. The method of claim 4 further comprising periodically recording
the windspeed and wind direction for wind power system site
survey.
8. The method of claim 4 further comprising modulating the laser
with a pseudorandom sequence, storing the received backscatter
radiation in a histogramming-type of memory, and correlating this
received backscattered radiation with the pseudorandom sequence to
obtain windspeed at least one particular distance from the tunable
laser.
9. The method of claim 8 further comprising scanning the laser
radiation to obtain windspeed and wind direction information at
multiple locations within a volume of air.
10. The method of claim 8 further comprising recording the
windspeed and wind direction for wind power system site survey.
11. The method of claim 9 further comprising determining blade
pitch for at least one blade of a wind turbine.
12. The method of claim 1 wherein the laser radiation is emitted
into the air from a location on a wind turbine.
13. The method of claim 12 wherein the location on the wind turbine
is on a hub or a nacelle of a wind turbine.
14. The method of claim 13 further comprising modulating the laser
with a pseudorandom sequence, storing the received backscatter
radiation in a histogramming-type of memory, and correlating the
received backscattered radiation with the pseudorandom sequence to
obtain windspeed at, at least one particular distance from the
tunable laser.
15. The method of claim 14 further comprising determining
windspeeds and wind directions at a plurality of altitudes, and for
determining blade pitch for the wind turbine in response to the
windspeeds and wind directions.
16. A system for optically sensing air data comprising: a tunable
laser for generating laser radiation; at least one beam splitter
for splitting the laser radiation into a projected component and a
control component; at least one optical notch filter; at least one
control component detector coupled to receive at least a portion of
the control component through the at least one optical notch filter
and generate an electronic control signal therefrom; apparatus for
projecting the projected component into the air to induce scattered
radiation and for receiving a portion of the scattered radiation as
backscattered radiation; at least one backscattered radiation
detector coupled to receive at least a portion of the backscattered
radiation through the at least one optical notch filter and
generate an electronic backscatter signal therefrom; control and
computing apparatus for sweeping a wavelength of the tunable laser
and for receiving the electronic backscatter signal and the
electronic control signal and determining Doppler shift therefrom,
and for processing the Doppler shift to determine wind speed.
17. The system of claim 16 further comprising: a pseudorandom
sequence generator for generating a pseudorandom sequence; a
modulator for modulating the laser radiation with the pseudorandom
sequence; and wherein the control and computing apparatus
correlates the pseudorandom sequence with the electronic
backscatter signal to determine the Doppler shift at a plurality of
ranges from the system.
18. The system of claim 17 wherein the control and computing
apparatus analyzes the electronic backscatter signal to determine
Rayleigh scattering, and to determine air temperature therefrom at
a plurality of ranges from the system.
19. The system of claim 18 further comprising a digital data
recorder, and wherein the digital data recorder is configurable to
record minimum, average, and peak-gust windspeed data with air
temperature data at least four times per hour.
20. The system of claim 19 wherein the digital data recorder is
configurable to record the minimum, average, and peak-gust
windspeeds with air temperature at least four ranges from the
system, and wherein the digital data recorder has storage capacity
for at least one month of recorded windspeed data.
21. The system of claim 17 wherein the control and computing
apparatus analyzes the electronic backscatter signal to determine
Rayleigh scattering, and to determine air temperature therefrom at
a plurality of ranges from the system.
22. The system of claim 21 wherein the apparatus for projecting the
projected component into the air to induce scattered radiation and
for receiving a portion of the scattered radiation as backscattered
radiation is adapted for scanning a volume of airspace.
23. The system of claim 22 further comprising control apparatus for
controlling at least one blade pitch of at least one wind
turbine.
24. The system of claim 23 wherein the control and computing
apparatus selectively ignores at least some of the backscattered
radiation to avoid reading blade motions of at least one wind
turbine as wind.
25. The system of claim 24 wherein the control and computing
apparatus determines which backscattered radiation to ignore by
comparing angle and range information with a location of the at
least one wind turbine.
26. The system of claim 23 wherein at least a portion of the system
is located within an element of a wind turbine selected from the
group consisting of a nacelle and a hub.
27. The system of claim 22 wherein the control and computing
apparatus is adapted for providing warning of wind conditions
selected from the group consisting of hazardous wind speeds, wind
shear, microbursts, and dust-devils.
28. The system of claim 22 wherein the control and computing
apparatus is adapted for providing warning of atmospheric
turbulence caused by events selected from the group consisting of
convective instability, terrain-induced flow irregularities,
obstacle-induced flow irregularities and wind forcing over rough
surfaces.
29. A system for optically sensing air data comprising: a
pseudorandom sequence generator for generating a pseudorandom
sequence; a tunable laser for generating laser radiation modulated
by the pseudorandom sequence; at least one beam splitter for
splitting the laser radiation into a projected component and a
control component; at least one optical notch filter; at least one
control component detector coupled to receive at least a portion of
the control component through the at least one optical notch filter
and generate an electronic control signal therefrom; apparatus for
projecting the projected component into the air to induce scattered
radiation and for receiving a portion of the scattered radiation as
backscattered radiation; at least one backscattered radiation
detector coupled to receive at least a portion of the backscattered
radiation through the at least one optical notch filter and
generate an electronic backscatter signal therefrom; and control
and computing apparatus for sweeping a wavelength of the tunable
laser, for receiving the electronic backscatter signal and the
electronic control signal, for correlating the pseudorandom
sequence with the electronic backscatter signal and determining
Doppler shift at a plurality of ranges therefrom; and wherein the
control and computing apparatus analyzes the electronic backscatter
signal to determine Rayleigh scattering, and to determine air
temperature therefrom at a plurality of ranges from the system.
30. The system of claim 29 wherein the laser radiation is directed
along a plurality of axes and wherein the control and computing
apparatus determines wind speed and direction at a plurality of
ranges from determined Doppler shift along the plurality of axes at
the plurality of ranges.
31. The system of claim 30 further comprising a digital data
recorder, and wherein the digital data recorder is configurable to
record minimum, average, and peak-gust windspeed data with air
temperature data at least four ranges from the system at least four
times per hour, and wherein the digital data recorder has storage
capacity for at least one month of windspeed data.
32. The system of claim 31 wherein the apparatus for projecting the
projected component into the air to induce scattered radiation and
for receiving a portion of the scattered radiation as backscattered
radiation is adapted for scanning a volume of airspace.
33. The system of claim 32 further comprising control apparatus for
controlling at least one blade pitch of at least one wind
turbine.
34. The system of claim 33 wherein the control and computing
apparatus filters windspeed data by comparing determined angle and
range information with angle and range information corresponding to
a location of at least one wind turbine to avoid reading blade
motion of the at least one wind turbine as wind.
35. The system of claim 34 further comprising control apparatus for
controlling at least one blade pitch of a second wind turbine.
36. The system of claim 35 wherein at least a portion of the system
is located within an element of a wind turbine selected from the
group consisting of a nacelle and a hub.
37. The system of claim 32 wherein the control and computing
apparatus is adapted for providing warning of wind conditions
selected from the group consisting of high wind speed hazards,
atmospheric turbulence, wind shear, microbursts, and dust-devils in
the area of interest.
38. The system of claim 32 wherein the control and computing
apparatus is adapted for providing warning of the wind conditions
approaching and within an aircraft approach path in the area of
interest.
39. The system of claim 32 wherein the system is located near an
airport, the area of interest comprises an airport traffic pattern
area, and the control and computing apparatus is adapted for
providing warning of hazardous wind conditions in the airport
traffic pattern area.
40. The system of claim 32 wherein the system is located, the area
of interest comprises an area near a highway, and the control and
computing apparatus is adapted for providing traffic alerts when
hazardous wind conditions are detected in the area of interest.
Description
CROSS-REFERENCE TO RELATED APPLICATIONS
[0001] This application claims benefit of priority to and is a
continuation-in-part of commonly-owned and copending U.S. patent
application Ser. No. 11/488,259. In turn, U.S. patent application
Ser. No. 11/488,259 claims benefit of priority to U.S. Provisional
Patent Application Ser. No. 60/699,630 filed Jul. 15, 2005. This
application is also a continuation-in-part of U.S. application Ser.
No. 11/103,020 filed 11 Apr. 2005, which is a continuation of U.S.
application Ser. No. 10/632,735 filed Aug. 1, 2003, now U.S. Pat.
No. 6,894,768, which claims benefit of priority to U.S. Provisional
Patent Application No. 60/400,462 filed Aug. 2, 2002. All of the
aforementioned applications are hereby incorporated by
reference.
BACKGROUND
[0003] An Air Data System ("ADS") provides sensed telemetry
informing pilots, navigators or Vehicle Management System computers
of air parameter(s) affecting aircraft stability. These air
parameters include, for example, air speed, air temperature and air
pressure, each being useful for navigation and flight control. The
ADS exists in many forms, for example, as mechanical,
opto-mechanical or opto-electronic devices.
[0004] An Optical Air Data System ("OADS") uses light to determine
parameters of air speed. The OADS transmits light pulses into the
atmosphere and receives light that aerosols reflect or
"backscatter" towards the aircraft. Aerosols are fine solids and/or
liquid particles suspended in air or other gases. The OADS may also
measure the Doppler effect by receiving backscattered light and
measuring its return frequency to determine speed. Certain prior
art OADSs rely on scattered light that is unpredictable because of
aerosol distributions that vary significantly with altitude and
cloud content. In addition, some regions of the atmosphere contain
too few aerosols to enable reliable air data measurements, and such
an OADS cannot determine air temperature or air pressure.
[0005] Ground-based air data measurements can also be of interest
in other applications such as wind measurements for weather
monitoring, weather prediction and traffic alerts.
[0006] Wind conditions near airports and on approach paths to
airports can be of great interest to pilots. In particular,
improved detection and measurement of wind shear, updraft,
downdraft, and microburst conditions has been of interest since a
microburst was blamed for the demise of a Lockheed L-1011 trying to
land at Dallas in 1985. Aircraft are particularly sensitive to such
wind conditions during the critical flight phases of takeoff and
landing; it is desirable to equip airports with devices for
detecting such conditions so that destruction of aircraft and death
of crew and passengers can be avoided.
[0007] Wind conditions are often measured at more than one point on
an airport in an attempt to detect potentially harmful wind
conditions. Since wind shear is characterized by a difference in
wind speeds and directions with altitude, it is also desirable to
measure wind conditions at several altitudes and not just near the
surface.
[0008] Tax and other incentives enacted by the United States and
several states have increased interest in obtaining electric power
from renewable energy sources, including wind power systems.
Detailed measurements of wind speed, air temperature, air
turbulence, and similar information at the surface and at altitudes
within a few hundred meters of the surface are of use in evaluating
locations for wind power systems. Further, realtime measurements of
wind conditions, turbulence, and temperature at the surface and at
altitude may be of use in controlling wind power systems and in
predicting updrafts and microbursts to help protect such systems
from adverse conditions.
SUMMARY
[0009] A method for sensing air includes using at least one, and at
times three, transceivers for projecting laser energy as laser
radiation to the air. When using three transceivers, the
transceivers are aligned along several different axes, when using
one transceiver the projected radiation may be scanned. Each
transceiver receives laser energy as it is backscattered from the
air. A computer processes signals from the one or more transceivers
to distinguish molecular scattered laser radiation from aerosol
scattered laser radiation and determines air temperatures, wind
speeds, and wind directions based on the scattered laser radiation.
Applications of the method to wind power site evaluation, wind
turbine control, weather monitoring, aircraft air data sensing, and
airport safety are presented. In some embodiments the laser energy
is scanned to cover a region of interest.
[0010] A system for optically sensing air data has a tunable laser
for generating laser radiation and a beam splitter for splitting
the laser radiation into a projected component and a control
component. A control component detector receives at least a portion
of the control component through an optical notch filter and
generate an electronic control signal. The projected component is
emitted into the air and a portion of scattered radiation is
received as backscattered radiation, a portion of which is received
through an optical notch filter into a backscattered radiation
detector to generate an electronic backscatter signal therefrom.
The wavelength of the tunable laser is swept and the control signal
and backscatter signal are compared to determine Doppler shift,
this is used to determine wind speed. In an embodiment, a
pseudorandom sequence generator modulates the laser radiation and
the electronic backscatter signal is correlated with the random
sequence to determine the Doppler shift at several ranges from the
system.
BRIEF DESCRIPTION OF THE DRAWINGS
[0011] FIG. 1 shows one Optical Air Data System ("OADS"), according
to an embodiment.
[0012] FIG. 2 shows one OADS, according to an embodiment.
[0013] FIG. 3 illustrates an exemplary air speed calculation with
an OADS, according to an embodiment.
[0014] FIGS. 4-7 show graphs illustrating exemplary calculations
for other air parameters with an OADS, according to an
embodiment.
[0015] FIG. 8 is a flowchart showing one exemplary method of
operation of an OADS, according to an embodiment.
[0016] FIG. 9 is a flowchart showing one exemplary method of
operation of an OADS, according to an embodiment.
[0017] FIG. 10 is a block diagram of an embodiment of the OADS
using the Random Modulated Continuous Wave approach to range
resolution.
[0018] FIG. 11 illustrates some wind conditions that can cause
hazard to aircraft near airports or to wind power systems.
[0019] FIG. 12 illustrates application to a wind power system.
[0020] FIG. 13 is a block diagram of an embodiment of an air data
system suitable for ground-based applications.
[0021] FIG. 14 illustrates an alternative embodiment of the
ground-based air data system.
[0022] FIG. 15 illustrates a scanning embodiment of the
ground-based air data system for mapping windspeed and temperature
around a location.
DETAILED DESCRIPTION OF THE EMBODIMENTS
[0023] FIG. 1 shows one Optical Air Data System ("OADS") 101
mounted on or within an aircraft 102. In this embodiment, OADS 101
is configured for projecting laser radiation 103 to air 104. Laser
radiation 103 impinges on air 104 and aerosol particles 105 (in air
104), causing scattering of laser radiation 103, which is
represented in FIG. 1 as a scatter field 106. Distance between
aircraft 102 and scatter field 106 is controlled by overlap between
laser radiation 103 and the transceiver 110 field of view at a
distance from aircraft 102, to provide an optimized intensity for
return laser radiation 107 and to eliminate possible measurement
error arising from displaced air proximate to aircraft 102. OADS
101 detects backscattered laser radiation 107 that is backscattered
from air 104 at laser scatter field 106. Radiation 107 may be in
the ultra-violet (UV) spectrum, for example, having a wavelength
within a range of 250 nm to 270 nm; however, other ranges may
alternatively be used to produce scatter field 106.
[0024] Return laser radiation 107 typically contains molecular
scattered (e.g., Rayleigh) components 107A and/or aerosol scattered
(e.g., Mie) components 107B. OADS 101 distinguishes the molecular
scattered components 107A from the aerosol scattered components
107B and correspondingly determines one or more air parameters
based on backscattered laser radiation 107. Examples of such air
parameters include air speed, air pressure, air temperature and/or
aircraft orientation angles relative to the local wind. OADS 101
may be configured with other aircraft as well, including unmanned
air vehicles (UAVs), helicopters, missiles, gliders and space
shuttles. Although illustrated within a "nose" 108 of aircraft 102,
OADS 101 may be configured in any other part of aircraft 102.
[0025] As shown in FIG. 1, OADS 101 includes a laser 109 configured
for generating laser radiation 103. Transceiver 110 is configured
for transmitting laser radiation 103, from laser 109 via optical
coupling 111, and receiving backscattered laser radiation 107.
Optical coupling 111 may exist in the form of a fiber optic
connection or free space transmission. Accordingly, transceiver 110
projects the laser radiation as laser radiation 103 to air 104. Air
104 scatters laser radiation 103 at scatter field 106 in a
plurality of directions (e.g., illustrated as vectors 112). Scatter
field 106 also returns, or backscatters, radiation 107 towards
transceiver 110, which subsequently receives the backscattered
laser radiation 107. Transceiver 110 converts backscattered laser
radiation 107 to processable electronic signals, via computer 113,
to determine the air parameters.
[0026] Computer 113 communicatively couples with transceiver 110
and processes signals from transceiver 110 to distinguish a
molecular-scattered component 107A from an aerosol-scattered
component 107B. Computer 113 determines the air parameters based on
laser radiation 107 backscattered from molecules and/or aerosols in
air 104. Accordingly, as described below, computer 113 may employ
one or more digital signal processing algorithms to determine such
parameters.
[0027] While OADS 101 illustrates one transceiver 110 in an
exemplary embodiment, a plurality of transceivers may be used,
depending on an application. For example, a missile employing OADS
101 may use two transceivers 110 to determine air parameters such
as a forward velocity (e.g., air speed) and a vertical plane, or
angle of attack", of the missile. An airplane may use three
transceivers 110 positioned in a particular manner to determine
various aircraft geometries, such as angle of attack and sideslip,
in addition to the air parameters of air speed, air pressure and
air temperature. In addition, air vehicles (fixed wing and rotary)
may employ three or more transceivers and/or lasers to increase
Optical Air Data System reliability through redundant system
architecture. Using three OADS transceivers mounted on three
non-coplanar axes may fully resolve a total airspeed vector by
providing three independent measurements for the air speed vector.
The transceivers are for example located in uncommon planes and
their geometry known respective of an aircraft centerline. Vector
algebra may then be used to determine the full airspeed vector,
including forward air speed, angle-of-sideslip and
angle-of-attack.
[0028] FIG. 2 shows one OADS 140. OADS 140 illustrates another
embodiment used for determining air parameters, such as those
described in FIG. 1, based upon laser radiation backscattered from
both air molecules and aerosols. In this embodiment, OADS 140
includes laser 141 configured for generating laser radiation 142.
Laser 141 may be a tunable laser having a tuned center wavelength
of about 253.7 nm, although other wavelengths may be used. For
example, laser 141 may be a frequency quadrupled, Nd:YAG (i.e.,
neodymium:yttrium-aluminum-garnet) pumped Ti:Sapphire
(titanium-sapphire) laser. Alternatively, frequency-quadrupled
Yb-doped (ytterbium-doped) fiber lasers may be used that offer
important benefits of smaller size, lighter weight, increased
robustness and improved reliability, as compared to Nd:YAG-pumped
Ti:Sapphire lasers. Alternately, diode lasers, diode laser bars,
stacks of diode laser bars and frequency up-conversion techniques
can be used to fabricate the laser. Laser 141 may generate laser
radiation that is tunable across a frequency range of about 40 GHz;
laser 141 may be a continuous wave laser, which sweeps in frequency
across this range, or it may be a pulsed laser controlled such that
each pulse has a frequency distribution centered about a tunable
peak frequency. In one embodiment, the peak frequency increments by
about 100 MHz from each pulse to the next. Laser 141 may tune+/-20
GHz about a center frequency of approximately 1182.5 THz, or
c/253.7 nm, where c is the speed of light (approximately
3.times.10.sup.8 m/s). In the illustrated embodiment, laser 141
radiates laser radiation 142 to beam splitter 143, which splits the
beam into two components, 143A and 143B. Component 143A is directed
through air 144; component 143B is directed to beam splitter
145.
[0029] In particular, component 143A of laser radiation 142
directed to air 144 is scattered into scatter field 146. Scattering
of component 143A is illustrated by scattering vectors 147 in
scatter field 146, whereas return scattering is illustrated by
backscattered laser radiation 148. Component 143B of the laser
radiation 142 is used as a reference for comparison to
backscattered laser radiation 148. Such a comparison is for example
useful in determining air parameters such as air speed, since
transmitted and received frequencies of the laser radiation may be
ascertained for use in a Doppler equation; such a process is
explained in greater detail herein below.
[0030] In the illustrated embodiment, backscattered laser radiation
148 is received through optics 149. In one example, optics 149 is a
telescope that gathers backscattered laser radiation 148 into a
beam 150. Optics 149 also directs beam 150 to beam splitter 151, to
split beam 150 into two components 150A/150B. Component 150B of
beam 150 passes through vapor filter 152 to detector 153 to produce
electronic signal 158 representative of the component 150B
impinging detector 153; whereas component 150A is directed by beam
splitter 151 to detector 154.
[0031] In one embodiment, detector 154 is a photodetector that
receives radiation 150A and converts it into an electronic signal
155. Detector 154 connects to a central computer 156 to process
electronic signal 155. Similarly, detector 153 is a photodetector
configured for detecting component 150B, which is filtered by vapor
filter 152 as filtered component 157. Detector 153 converts
component 157 to an electronic signal 158 for processing by central
computer 156.
[0032] Accordingly, electronic signal 158 corresponds to
backscattered laser radiation 148 as filtered by vapor filter 152;
and electronic signal 155 corresponds to unfiltered backscattered
laser radiation 150A. Electronic signal 155 is thus used to nullify
certain anomalies as computer 156 processes electronic signal 158.
For example, when processed with electronic signal 158, signal 155
may be used to remove, from signal 158, certain laser transmission
power fluctuations in filtered component 157 caused by atmospheric
changes in air 144. Such a process is explained in more detail in
connection with FIGS. 4-7.
[0033] Computer 156 includes lookup tables 170 and 172 that may be
utilized to determine temperature and/or pressure as discussed
below.
[0034] Reference component 143B of the laser radiation 142 is split
into two components 159 and 160 by beam splitter 145. Component 160
is directed by beam splitter 145 to vapor filter 152 via mirrored
surface 161, to measure filter characteristics, whereas component
159 is directed by beam splitter 145 to detector 162, to generate
electronic signal 163. Electronic signal 163 is for example used to
normalize power fluctuations in the return of backscattered laser
radiation 148 caused by power fluctuations in the generation of
laser radiation 142 by laser 141. Such a process is explained in
more detail in FIGS. 4-7.
[0035] Vapor filter 152 filters component 160 to produce filtered
component 164. Filtered component 164 is directed to detector 165,
via mirrored surface 166, and then converted to an electronic
signal 167. Central computer 156 processes electronic signal 167 to
determine filter characteristics, such as frequencies and
suppression features of the band stop region of vapor filter 152.
One such process is also explained in more detail in context of
FIGS. 4-7.
[0036] While FIG. 2 shows OADS 140 as having free space optical
transmission and optical components such as beam splitters 143, 145
and 151 and mirrors 161 and 166, optical fiber may be used for
laser 141 transmission along paths 142, 143A, 143B, 159, 160, 164,
150, 150A, 150B and/or 157; in such an embodiment, fiber splitters
may be used in place of beam splitters 143, 151 and 145, and
mirrors 161 and/or 166 may be eliminated.
[0037] It will also be appreciated that although the embodiment
shown in OADS 140 of FIG. 2 employs vapor filter 152, other types
of filters may be utilized. For example, notch or optical notch
filters such as interference filters, dichroic filters, fiber Bragg
grating filters, volume holographic gratings, and/or Rugate filters
may be utilized. A filter used in place of vapor filter 152 may
advantageously have properties such as: (1) high optical absorption
within a stop-band region on the order of 40-60 dB or more; (2) a
notch filter absorption width between about 5 GHz and 100 GHz, with
an absorption width under 10 GHz being preferred; and (3) steep
absorption sidewalls, with a 10%-90% absorption transition
occurring within about 5 GHz or less. Pass-band filters may also be
used. Single filters with multiple absorption features may be
utilized or optical or fiber splitters may be used to route optical
signals through multiple filters, each filter having a single
absorption feature.
[0038] Filters other than atomic vapor filters may provide certain
advantages. For example, while the absorption frequencies of atomic
vapor filters are reliably tied to properties of an atomic vapor
used, their use may constrain an OADS to include a tunable laser
having output at such frequencies. However, certain tunable lasers
may have improved performance and/or stability at frequencies that
do not conveniently match atomic vapor filter absorption
frequencies. In particular, Bragg grating filters are a low cost,
optical notch filter effective for airspeed measurement at longer
wavelengths such as 1550 nm. Certain filters such as interference
filters, dichroic filters, fiber Bragg grating filters, volume
holographic grating filters, and/or Rugate filters may be designed
to have absorption features tuned to a preferred frequency output
range of a tunable laser, rather than tuning the laser to the
filter. The use of a tunable laser, and a matching notch filter in
an OADS may thus (1) enable use of higher laser output power for
improved return signal strength, (2) make the OADS more robust with
respect to thermal stability, vibration and shock, (3) eliminate
hazardous materials (e.g., mercury) from the OADS, and/or (4)
reduce size, weight and/or cost of the OADS.
[0039] FIG. 3 shows one graph 200 useful in illustrating an
exemplary air speed calculation with OADS 140. Graph 200 shows two
curves, 201 and 202, comparing normalized laser radiation
magnitudes as a function of frequency (signal strength, that is,
normalized laser radiation magnitude, is plotted with respect to
axis 205, and frequency is plotted with respect to axis 204). Curve
202 exemplifies filtered radiated laser radiation such as that of
filtered component 164 of FIG. 2. As such, curve 202 shows filter
characteristics of vapor filter 152 of FIG. 2 determined by
processing of electronic signal 167. Curve 202 shows peak
absorption of filter 152 occurring at a down-translated frequency
of 0 GHz. By way of example, the actual peak absorption frequency
of filter 152 may be about 1182.5 THz (i.e., having a corresponding
wavelength of about 253.7 nm).
[0040] Laser radiation 142 generated by laser 141 passes through
filter 152 to provide filtered component 164. Once filtered
component 164 is converted to electronic signal 167 by detector
165, computer 156 analyzes and stores features of vapor filter 152
through digital signal processing of signal 167 (e.g., computer 156
stores reference features, obtained under controlled conditions,
for use in future calculations). As shown in this example, features
of vapor filter 152 have approximately 10% normalized absorption at
approximately +/-5 GHz (i.e., 0.9 normalized transmission factor at
approximately +/-5 GHz according to axis 205) about the peak
absorption frequency. Other types of suitable filters may include
different absorption/transmission features.
[0041] Curve 201 exemplifies filtered backscattered laser radiation
such as that of filtered component 157 of FIG. 2. In one
embodiment, curve 201 is used to determine air speed by comparison
to curve 202. For example, curve 202 illustrates how vapor filter
152 affects laser radiation 142; curve 201 similarly illustrates
how vapor filter 152 affects laser radiation 142 as laser radiation
142 is backscattered (e.g., returns as radiation 148) from air 144.
Frequency shift 203 represents the change in frequency of peak
absorption for vapor filter 152 between transmitted laser radiation
142 and returned laser radiation 148. Computer 156 processes
algorithms applying Doppler velocity equation to determine air
speed from frequency shift 203.
[0042] To determine air speed in one embodiment, computer 156
determines how far in frequency the peak absorption frequency of
filtered component 157 has shifted from the initial laser frequency
by comparing curve 202 to curve 201 (e.g., comparing peak
absorption frequencies of filtered components 157 and 164).
Frequency shift 203 substantially equates to a radial wind velocity
through the Doppler velocity equation:
.DELTA. v D = 2 V R .lamda. , ( Eq . 1 ) ##EQU00001##
where .DELTA..nu..sub.D represents the Doppler frequency shift,
V.sub.R represents velocity component of the vehicle (e.g.,
aircraft 101 of FIG. 1) along the laser direction of propagation
143A and .lamda. represents the wavelength of laser radiation
142.
[0043] In one embodiment, wind velocity component V.sub.R may be
measured by determining the frequency shift from curve 202 of graph
200 as compared to curve 201 of graph 200. This is accomplished by
calculating a symmetry point of each curve 201 and 202 and
determining a difference in symmetry points between the two
curves.
[0044] Vapor filter 152 may have a plurality of absorption
features. Consequently, OADS may have a plurality of absorption
maxima, such as those illustrated by curves 201 and 202 of FIG. 3,
which may be used to provide a more accurate estimate of the
vehicle's velocity. The vehicle's velocity V.sub.R may be
calculated using equation 1 for each absorption feature. An average
velocity of the vehicle may then be calculated from each value of
V.sub.R.
[0045] FIGS. 4-7 show graphs illustrating exemplary calculations
for other air parameters with OADS 140. For example, after
determining frequency shift due to air speed as shown in FIG. 3,
other air parameters such as air temperature and air pressure may
be calculated. In one example, computer 156 initially determines an
intensity measurement of the detected backscattered laser radiation
(e.g., filtered component 157 detected by detector 153) from
electronic signal 158. This experimentally verified intensity
measurement of returned laser radiation corresponds to the
following equation:
S S ( v ) = P L T L D S T R E S .intg. v r .intg. v laser [ L ( v
laser ) F ( v r - v ) ( rR ( v r - ( v laser - .DELTA. v D ) ) + mM
( v r - ( v laser - .DELTA. v D ) ) ) ] ( Eq . 2 ) ##EQU00002##
where S.sub.S(.nu.) is electronic signal 158 from detector 153;
P.sub.L is the laser power, T.sub.L is the transmission coefficient
through air 144 along laser path 143A, L(.nu..sub.laser) is the
laser line shape inherent to the laser 141 output as a function of
laser frequency .nu..sub.laser, T.sub.R is the transmission
coefficient through air 144 along laser path 148, E.sub.S is
optical efficiency of the detector channel through detector 153,
F(.nu.) is the band stop frequency range of vapor filter 152
centered at a frequency of .nu., R is Rayleigh scattering as a
function of frequency (applicable to the Rayleigh regime)
.nu..sub.r for backscattered laser radiation minus the quantity of
laser frequency .nu..sub.laser minus the Doppler shift
.DELTA..nu..sub.D, r is the Rayleigh scattering magnitude
coefficient dependent on air density and the Rayleigh
backscattering coefficient, M is Mie scattering as a function of
.nu..sub.r minus the quantity of .nu..sub.laser minus
.DELTA..nu..sub.D, m is the Mie scattering magnitude coefficient
dependent on aerosol concentration and the Mie backscattering
coefficient, and D.sub.S is detector 153 efficiency. The Rayleigh
backscattering coefficient r and the Mie backscattering coefficient
m are constant for a particular atmosphere. These coefficients
correspond to the number of scatterers (i.e., molecules for
Rayleigh, aerosols for Mie) per unit volume of atmosphere.
[0046] Next, computer 156 may determine other air parameters,
utilizing the result obtained for the measured intensity of the
returned laser energy. Such a process, for example, may begin by
determining characteristics of vapor filter 152 by transmitting of
reference laser radiation 160 through vapor filter 152. For
example, measuring band stop characteristics of vapor filter 152
with laser 141 (e.g., via component 143B to electronic signal 167)
during experimentation yields a convolution of the laser wavelength
and the filter according to the following equation:
S F ( v ) = P L E F D F .intg. v laser [ L ( v laser ) F ( v laser
- v ) ] , ( Eq . 3 ) ##EQU00003##
where S.sub.F(.nu.) is signal 167 from detector 165 as a function
of frequency .nu. (e.g., as illustrated in curve 221 of FIG. 4);
E.sub.F is the optical efficiency of filter 152 collection along
paths 160 and 164, and D.sub.F is detector 165 efficiency.
[0047] Note that all optical efficiencies E.sub.F and E.sub.S
capture signal losses that are optical in nature. For example,
E.sub.F, the optical efficiency for detector 165, includes the
optical beam splitting ratios for beam splitters 143 and 145, the
optical transmission and coupling across filter 152 and the optical
delivery efficiency onto detector 165. E.sub.s, the optical
collection efficiency for detector 153, includes the collection
efficiency of telescope 149, the optical coupling efficiency into
path 150, the beam splitter ratio of beam splitter 151, the
transmission efficiency across filter 152 and the delivery
efficiency onto detector 153. Detector efficiencies D.sub.F and
D.sub.S include the detector conversion efficiencies for detectors
165 and 153, respectively. Thus, D.sub.F is the conversion
efficiency whereby detector 165 converts laser radiation along path
164 into an electrical signal 167. Likewise, D.sub.S is the
conversion efficiency whereby detector 153 converts laser radiation
along path 157 into an electrical signal 158.
[0048] Backscattered laser radiation 148 may include power
fluctuations that are caused by laser 141 while generating laser
radiation 142. Accordingly, laser radiation detected by detector
162 (e.g., via component 159) may be utilized to normalize power
fluctuations attributable to laser 141. In one embodiment, detector
162 converts component 159 into electronic signal 163. In turn,
computer 156 processes and normalizes according to the following
equation:
S.sub.L(.nu.)=P.sub.LE.sub.LD.sub.L.intg.d.nu.L(.nu.), (Eq. 4)
where S.sub.L(.nu.) is the electronic signal 163 from detector 162,
E.sub.L is the optical collection efficiency for detector 162,
D.sub.L is the conversion efficiency of detector 162 and P.sub.L is
the power of laser 141. Note that the optical collection efficiency
E.sub.L includes the beam splitting ratios of beam splitters 143
and 145 and the delivery efficiency of laser beam path 159 onto
detector 162.
[0049] Curve 221 of graph 220 of FIG. 4 represents the magnitude of
laser radiation (component 164) filtered by vapor filter 152 and
normalized between 0 and 1. Curve 221 represents the magnitude of
the laser radiation as a function of frequency (i.e., laser
radiation magnitude plotted with respect to axis 222 and frequency
plotted with respect to on axis 223). Curve 221, therefore,
illustrates filtered laser radiation via component 160 as
determined by computer processing of electronic signal 167, plotted
as laser radiation magnitude normalized between 0 and 1, versus
frequency.
[0050] In one embodiment, absorption/transmission characteristics
of vapor filter 152 are normalized using Eq. 3 and Eq. 4. Eq. 3
yields stop band characteristics of filter 152 and Eq. 4 accounts
for power fluctuations in the generation of laser radiation 142.
With the power fluctuations of Eq. 4 substantially removed, a
"normalization channel" is created, and power fluctuations
attributable to atmospheric changes may be accounted for.
[0051] In one embodiment, additional power fluctuations caused by
atmospheric changes in air 144 are also removed. For example, laser
radiation detected by detector 154 (e.g., via component 150A)
assists in removing laser power fluctuations caused by atmospheric
changes in air 144. Accordingly, detector 154 converts received
laser radiation into electronic signal 155. Computer 156, in turn,
processes electronic signal 155 to determine the normalized laser
radiation magnitude according to the following equation:
S N = P L T L T R E N D N .intg. v .intg. v laser [ L ( v laser ) (
rR ( v - ( v laser - .DELTA. v D ) ) + mM ( v - ( v laser - .DELTA.
v D ) ) ) ] ( Eq . 5 ) ##EQU00004##
where S.sub.N is the signal 155 from detector 154; E.sub.N is
optical collection efficiency of the detector 154 and D.sub.N is
the conversion efficiency of detector 154.
[0052] In one embodiment, it is advantageous to normalize the
various characteristic functions to enable a closed-loop solution
to the process of determining temperature and pressure. In one
example, therefore, computer 156 calculates the normalized laser
line shape according to following equation:
.intg.L(.nu..sub.laser)d.nu..sub.laser=1, (Eq. 6)
where (as before) .nu..sub.laser is laser line shape frequency and
L denotes the laser line shape as a function of frequency. In
another example, computer 156 calculates normalized Rayleigh
Function according to the following equation:
.intg.R(.nu..sub.r)d.nu..sub.r=1, (Eq. 7)
where R denotes the Rayleigh line shape as a function of frequency
.nu..sub.r, applicable to the Rayleigh regime. In another example,
computer 156 scales the electronic signal 167 recorded from
detector 165 by dividing all recorded values by the maximum value
according to the following equation:
MAX(S.sub.F(.nu.))=1, (Eq. 8)
where MAX denotes an operation that finds a maximum value of a
particular function, and S.sub.F denotes electronic signal 167
measured from detector 165, as a function of frequency .nu. (e.g.
as illustrated in curve 221 of FIG. 4). In another example,
computer 156 normalizes the Mie Function according to the following
equation:
M(.nu.)=.delta.(.nu.), (Eq. 9)
where .delta.(.nu.) is the delta function.
[0053] In one embodiment, dividing the signal 167 collected from
detector 165 (and represented by Eq. 3, above) by the signal 163
collected from detector 162 (and represented by Eq. 4, above)
removes laser 141 power fluctuations, as follows:
S F ( v ) S L ( v ) = P L E F D F .intg. v laser [ L ( v laser ) F
( v laser - v ) ] P L E L D L .intg. vL ( v ) ( Eq . 10 )
##EQU00005##
Equation 10 simplifies to:
S F ( v ) S L ( v ) = E F D F E L D L L F ( v ) ( Eq . 11 )
##EQU00006##
where LF(.nu.) represents a convolution of functions L and F (that
is, a function that represents the effects of functions L and F
combined at each frequency .nu.).
[0054] In one embodiment, tuning the laser 141 to a reference
frequency .nu..sub.ref far enough removed from the effects of the
vapor filter 152 enables the measurement of the ratio of the
optical and detector efficiencies of the signal channels 167
(S.sub.F, represented by Eq. 3 above) and 163 (S.sub.L, represented
by Eq. 4 above). This, in turn, enables the normalization of the
signal 167 measurement to one, for simultaneously checking for
laser, detector and filter abnormalities on a scan-by-scan
basis:
S F ( v ref ) S L ( v ref ) = E F D F E L D L ( Eq . 12 )
##EQU00007##
[0055] In one embodiment, LF(.nu.) are determined to generate a
look up table of the convolution of theoretical Rayleigh functions
(calculated in terms of temperature and pressure) with the measured
filter function. Since the measured filter function is already the
convolution of the laser and filter spectra, convolving the
Rayleigh function with the measured filter signal 167 yields the
expected return signal from an atmosphere of pure Rayleigh
scatterers.
[0056] In one embodiment, the measured signal 158, which is the
backscatter return from the atmosphere 144 that passes through the
vapor filter 152 (and is represented by Eq. 2 above), is divided by
the signal 155, which is the backscatter return from the atmosphere
144 that does not pass through vapor filter 152 (and is represented
by Eq. 5 above). This calculation removes changes in signal
transmission that are independent of the factors to be
measured:
S S ( v ) S N ( v ) = P L T L D S T R E S .intg. v .intg. v laser [
( L ( v laser ) F ( v r - v ) ) ( rR ( v r - ( v laser - .DELTA. v
D ) ) + mM ( v r - ( v laser - .DELTA. v D ) ) ) ] P L T L T R E N
D N .intg. v .intg. v laser [ L ( v laser ) ( rR ( v r - ( v laser
- .DELTA. v D ) ) + mM ( v r - ( v laser - .DELTA. v D ) ) ) ] ( Eq
. 13 ) ##EQU00008##
Since M is a delta function, Equation 13 simplifies to:
S S ( v ) S N ( v ) = [ E S D S E N D N ] rLFR ( v laser - .DELTA.
v D ) + mLF ( v laser - .DELTA. v D ) r + m ( Eq . 14 )
##EQU00009##
where LFR(.nu.) represents a convolution of functions L, F and R in
the sense of the convolution LF(.nu.) discussed above.
[0057] In one embodiment, tuning laser 141 to reference frequency
.nu..sub.ref far enough removed from the effects of the vapor
filter 152 enables the measurement of the ratio of the optical and
detector efficiencies of the signal channels 158 (S.sub.S as
represented by Eq. 2 above) and 155 (S.sub.N as represented by Eq.
5 above). This enables a check for abnormalities in the filter on a
scan-by-scan basis:
S S ( v ref ) S N ( v ref ) = E S D S E N D N ( Eq . 15 )
##EQU00010##
[0058] In one embodiment, a variable K.sub.ref may be defined
as:
K ref = S S ( v ref ) S N ( v ref ) ( Eq . 16 ) ##EQU00011##
[0059] Once both data sets (i.e., S.sub.S and S.sub.N) are
symmetric about the same data point, computer 156 calculates
temperature and pressure from the return signal. Initially,
computer 156 uses theoretical Rayleigh functions that are functions
of temperature and pressure in conjunction with the measured filter
transmission to generate a lookup table 170 that stores laser,
Rayleigh, and filter (LFR(.nu.)) convolutions that are dependent on
atmospheric temperature and pressure. Computer 156 may then compare
a normalized return signal to a value stored in lookup table 170 to
determine atmospheric temperature and pressure. In order to compare
the return signal with the lookup table 170, computer 156 accounts
for the magnitude of Mie scatterers as well as any changes in air
density that may change the magnitude of the Rayleigh signal.
[0060] A vapor filter may be used as a bandstop filter; such
filters typically provide frequency stability, optical depth, and
optimal filter shape. For the purposes of separating the Rayleigh
and Mie scattering, an optical depth of approximately 60 dB
provides excellent absorption of Mie scattering within a small
frequency variance around .nu..sub.0(i.e., where .nu..sub.f is a
normalized frequency of 0 GHz). For example, an atomic vapor filter
may provide 60 dB of absorption in a frequency region that is not
contaminated by Mie scattering. This region may be used in
acquiring initial estimates of pressure and temperature (explained
below in FIG. 5). Such absorption is observable in FIG. 5 below as
the measured signal S.sub.F which has the magnitude of zero
centered about .nu..sub.0. This data provides information about
pure Rayleigh scattering that may be used to calculate the ratio of
Mie scattering to Rayleigh scattering, as shown in Eq. 17:
S S ( v 0 ) S N ( v 0 ) = [ E S D S E N D N ] rLFR ( v 0 ) + mLF (
v 0 ) r + m ( Eq . 17 ) ##EQU00012##
Since the vapor filter fully attenuates the Mie scattering in this
region:
S S ( v 0 ) S N ( v 0 ) = [ E S D S E N D N ] rLFR ( v 0 ) r + m ,
( Eq . 18 ) ##EQU00013##
where LFR(.nu..sub.0) is the value of the theoretical return signal
at particular atmospheric temperature and pressure. Accordingly,
computer 156 calculates the ratio of Mie scattering by first
defining a variable K.sub.0 as follows:
K 0 = S S ( v 0 ) S N ( v 0 ) ( Eq . 19 ) ##EQU00014##
and then solving for the ratio
m r = K 0 K a LFR ( v 0 ) - 1 ( Eq . 20 ) ##EQU00015##
Using the normalized signal return in the region of interest (i.e.,
the sloped region between the minimum and maximum of the signal
return) and writing the result in terms of the ratio of m over r,
yields the following:
S S ( v ) S N ( v ) = K a LFR ( v ) + m r LF ( v ) 1 + m r ( Eq .
21 ) ##EQU00016##
Substituting the ratio of m and r of Eq. 20 into Eq. 21 yields:
S S ( v ) S N ( v ) = K a LFR ( v ) LFR ( v 0 ) + LF ( v ) [ 1 - K
0 K a LFR ( v 0 ) ] ( Eq . 22 ) ##EQU00017##
Solving for LFR(.nu.) yields:
LFR ( v ) = S S ( v ) S N ( v ) LFR ( v 0 ) K a + LF ( v ) [ 1 K a
- LFR ( v 0 ) K 0 ] , ( Eq . 23 ) ##EQU00018##
where the measured signal return LFR(.nu.) is written in terms of
measured quantities and the theoretical values of LFR(.nu..sub.0)).
Computer 156 then calculates LFR(.nu.) and compares it to the
lookup table 170 to determine atmospheric temperature and pressure,
described in greater detail in FIG. 5.
[0061] Accounting for power fluctuations, optical efficiencies and
detector efficiencies as described herein allows for an independent
check on vapor filter 152 while OADS 140 operates. With variable
characteristics of detector channels and power fluctuations
accounted for, computer 156 may determine, for example, the
substantially constant characteristics of vapor filter 152, such
that more accurate measurements of received backscattered laser
radiation (e.g., laser radiation 148) are obtained.
[0062] In one embodiment, the normalization channel depicted in
FIG. 4 is used to remove atmospheric power fluctuations of laser
radiation 148. In doing so, computer 156 measures Rayleigh and Mie
components of laser radiation 147 in terms of optical efficiencies
and detector efficiencies. Such efficiencies are typically measured
on a shot-by-shot basis during the analysis process. In an
exemplary embodiment of operation, laser 141 generates and
transmits laser radiation 142 as a series of pulses at a particular
pulse repetition frequency ("PRF"), while in other embodiments
laser 141 is a continuous wave laser (as discussed in connection
with FIG. 2). Computer 156 then measures the Rayleigh and Mie
components in terms of optical efficiencies and detector
efficiencies on a pulse-by-pulse basis.
[0063] To measure Rayleigh components and Mie components, in one
embodiments OADS 140 tunes the frequency of the laser radiation 142
transmitted by laser 141. For example, laser 141 transmits the
laser radiation 142 at distal frequencies from the peak absorption
frequency of filter 152 (illustrated by .nu..sub.f in FIG. 4) to
provide a frequency-independent measurement. Computer 156 then
determines the line shape of laser radiation 142 through filter
152.
[0064] In one embodiment, measured intensity of the detected
backscattered laser radiation (e.g., as determined by electronic
signal 158) is functionally compared to normalized atmospheric
factors. The measured intensity often depends upon Mie scatterers
(e.g., aerosols) and air density changes due to altitude changes
and temperature changes. The air density changes and the
temperature changes are not, however, removed through the
normalization processes described herein. For computer 156 to
accurately determine air parameters such as temperature and
pressure of air 144, air density changes are removed from the
detected backscattered laser radiation so that computer 156 may
accurately determine the air parameters.
[0065] FIG. 5 shows graph 240 with curves 241 (detected
backscattered laser radiation at a higher air density causing both
Rayleigh and Mie scattering), 242 (detected backscattered laser
radiation at an air density causing Rayleigh scattering) and 243
(normalized Rayleigh scattering). Curves 241, 242 and 243
illustrate laser radiation magnitudes (plotted with respect to axis
250) as a function of frequency (plotted with respect to axis 251).
In one embodiment, computer 156 processes data from curves 241, 242
and 243 to determine other air parameters. For example, Mie
scattering effects are substantially isolated and removed from
calculations to determine air temperature and air pressure, since
these Mie scattering effects produce inaccurate measurements due to
inconsistent aerosol concentrations.
[0066] In one embodiment, to determine the air temperature and air
pressure, computer 156 processes the data from curves 241, 242 and
243 to substantially isolate and remove the Mie scattering effects,
such as those found in curve 241. In processing the data from
curves 241, 242 and 243, computer 156 calculates lookup table 170
in substantially real time using a measured laser/filter profile
(i.e., as measured at detector 165 of FIG. 2) convolved with
theoretical Rayleigh functions for a particular temperature and
pressure (e.g., illustrated by curves 242 and 243). Computer 156
then scales the measured return signal LFR(.nu.) (i.e., illustrated
by curve 241 in this example) with the ratio of m to r determined
by Eq. 20. Computer 156 then analyzes data near the deepest portion
of the filter attenuation (i.e., approximately +/-0.5 GHz from
.nu..sub.f) to estimate pressure and/or temperature. This portion
corresponds to a 60 dB region of absorption that is not
contaminated by Mie scattering. Use of this region is a preferred
aspect of the calculation technique that provides temperature and
pressure accuracy by providing a reliable temperature base from
which to increment temperature and/or pressure estimates.
[0067] Computer 156 calculates theoretical Rayleigh return assuming
an initial temperature estimate and performs a Least Square Error
(LSE) calculation to determine the accuracy of the temperature with
respect to the theoretical Rayleigh function. Computer 156 repeats
the process with incremental changes to temperature and/or pressure
until an optimal fit (i.e., an LSE calculation that corresponds to
design specifications) is achieved. Although discussed in detail
with respect to LSE, other approximation methods, such as
Newton-Raphson and Monte Carlo, may be used in alternative
embodiments. Accordingly, this disclosure teaches by way of example
and not by limitation.
[0068] Temperature affects air density in a manner that is
reciprocal to pressure; increasing pressure increases density,
while increasing temperature decreases density. Additionally,
increasing temperature increases the Rayleigh lineshape width while
increasing pressure increases the Rayleigh lineshape height.
Accordingly, for each incremental value of temperature and/or
pressure, the Rayleigh lineshape is unique. Such scattering theory
is discussed in "On The Kinetic Model Description Of
Rayleigh-Brillouin Scattering From Molecular Gases", G. C. Tenti,
D. Boley and R. C. Desai, Canadian Journal of Physics, vol. 52, pg.
285-290 (1974).
[0069] In one example, computer 156 determines air density changes
by aligning peak absorption frequencies of curves 241, 242 and 243,
illustrated at frequency .nu..sub.f. Since curve 243 represents
detected backscattered laser radiation containing substantially no
Mie scattering, curve 243 may be used as a reference where Mie
scattering has been eliminated. In one example, computer 156,
therefore, uses curve 243 to remove the effects of Mie scattering
by aligning curves 241, 242 and 243 and by calculating a ratio of
the detected backscattered laser radiation to theoretically pure
Rayleigh scattering (the ratio of curves 241 and 242) which may be
utilized to determine air density. Mie scattering effects are then
removed by subtracting curve 243 from the calculated ratio of
curves 241 and 242. With Mie scattering essentially removed from
the measurement, computer 156 more accurately determines air
temperatures and air pressures.
[0070] FIGS. 6 and 7 show other exemplary graphs that may be used
in determining air pressure and air temperature. FIG. 6 illustrates
a graph 260 of electronic signals 163 and 167 of FIG. 2
respectively generated by detectors 162 and 165 of FIG. 2. Graph
260 shows electronic signals 163 and 167, that represent light
intensity as a function of normalized signal strength (axis 261),
versus frequency (axis 262). FIG. 7 illustrates a graph 280 of
electronic signals 158 and 155 (see FIG. 2) generated by detectors
153 and 154 respectively, representing light intensity as a
function of normalized signal strength (axis 281), versus frequency
(axis 282). These four light intensities (represented by electronic
signals 163, 167, 158 and 155) may be measured, over time, through
transmission and collection of light corresponding to laser pulses,
or they may be measured through transmission and collection of
light corresponding to a continuous wave laser whose frequency
varies continuously. In one example, a transmission frequency of
laser radiation 142 of FIG. 2 generated by laser 141 at a certain
PRF may sweep such that each laser pulse is emitted at a different
frequency. Electronic signals 163 and 167 therefore illustrate how
laser radiation 142 of laser 141 may sweep in frequency across an
absorption band 263 of the vapor filter 152. Illustratively, FIG. 6
shows one complete frequency sweep of laser radiation 142 generated
by laser 141 and detected by detectors 162 and 165. Similarly,
electronic signals 155 and 158 of FIG. 7 show detected signals of
detectors 153 and 154 as laser radiation 142 of laser 141 performs
a complete sweep in frequency across absorption band 283 of vapor
filter 152.
[0071] From signals 163 and 167, computer 156 may for example
determine a normalized filter transmission, by dividing discrete
points of electronic signal 167 by corresponding discrete points of
signal 163. Similarly, computer 156 may determine a normalized
atmospheric return though vapor filter 152 by dividing discrete
points of signal 158 by corresponding discrete points of signal
155. These discrete points, described herein, correspond to
individual pulses of laser radiation 142.
[0072] Using normalized calculations of filter transmission (e.g.,
from graph 260) and the normalized calculations of atmospheric
return (e.g., from graph 280), computer 156 determines relative
optical efficiencies in the vapor filter 152.
[0073] In one embodiment, computer 156 determines optical
transmission for vapor filter 152 using the frequency independent
components of data from graph 260, FIG. 6 (there is substantially
no change in amplitude for signals 163 and 167 at frequencies
greater in magnitude than .+-.18 GHz from 0 GHz illustrated at
points 264, 265, 266 and 267). Computer 156 therefore determines a
ratio of optical transmission for vapor filter 152 by calculating a
ratio of signal 167 to signal 163, via frequency corresponding
points of the signals, for points representing frequencies greater
in magnitude than .+-.18 GHz from 0 GHz.
[0074] Similarly, computer 156 determines a magnitude of intensity
of atmospheric-returned laser radiation received through vapor
filter 152 using the frequency independent parts of the data from
graph 280, FIG. 7 (there is substantially no change in amplitude
for signals 155 and 158 at frequencies greater in magnitude than
.+-.18 GHz from 0 GHz illustrated at points 284, 285, 286 and 287).
Computer 156 thereby determines a ratio of atmospheric return with
the laser power measurement by calculating a ratio of signal 158 to
signal 155 via frequency corresponding points of the signals for
points representing the frequencies greater in magnitude than
.+-.18 GHz from 0 GHz.
[0075] In one embodiment, computer 156 calculates a ratio of signal
158 to signal 155 for frequencies between .+-.0.5 GHz (illustrated
at points 288 and 289). Such a frequency range includes
substantially no Mie scattering of laser radiation 142 for air 144;
it thus corresponds to substantially pure Rayleigh scattering.
Computer 156 thus compares a Rayleigh to Mie scattering strength
based upon the ratio of signal 158 to signal 155. Computer 156
determines Rayleigh to Mie scattering strength by comparing a ratio
of signal 158 to signal 155 at frequencies between .+-.0.5 GHz to
the ratio of signal 158 to signal 155 at frequencies greater than
.+-.18 GHz from 0 GHz. In one embodiment, computer 156 performs
similar calculations for "non-scattered" laser radiation 142 (e.g.,
component 143B of FIG. 2) based on data illustrated in FIG. 6 using
points 268 and 269. Such a process is further described in FIG.
8.
[0076] Ratios determined for the non-scattered laser radiation 142
and for the scattered laser radiation 148 may be used in tandem to
numerically calculate Laser-Rayleigh-Filter convolution (e.g.,
LRF(.nu.)) from data. The Laser-Rayleigh-Filter convolution is in
turn compared to a look up table of theoretical
Laser-Rayleigh-Filter convolution values to determine temperature
and pressure.
[0077] FIG. 8 shows a flowchart of one exemplary methodical
operation 400 of an OADS. Method 400 may be partially or fully
performed by computer 156 of OADS 140; computer 156 may receive
operating instructions from software and/or firmware. A laser
(e.g., laser 141 of FIG. 2) sweeps laser radiation across a
predetermined frequency spectrum, in step 401. The laser may sweep
the laser radiation across a frequency range of about +/-20 GHz by
transmitting laser radiation at a certain PRF (or it may sweep
frequency continuously, as discussed in connection with FIG. 2
above). In one embodiment, the PRF is about 1 kHz, with a pulse
width between about 50 ns and 100 ns, and a swept frequency range
is centered about a frequency corresponding to a peak absorption
frequency (e.g., 260 nm) of a filter (e.g., vapor filter 152, FIG.
2).
[0078] Laser radiation is typically split into four distinct paths
such that the laser radiation may be detected as four different
inputs, in step 402. These four paths of laser radiation correspond
to: 1) laser radiation transmitted by the laser (e.g., component
159 of FIG. 2); 2) laser radiation transmitted by the laser through
the filter (e.g., component 164 of FIG. 2); 3) laser radiation
transmitted by the laser into the air and backscattered (e.g.,
component 150A of FIG. 2); and 4) laser radiation transmitted by
the laser into the air and backscattered through the filter (e.g.,
component 157 of FIG. 2). For simplicity, these components are
hereinafter referred to as: 1) unfiltered laser radiation; 2)
filtered laser radiation; 3) unfiltered backscattered laser
radiation or unfiltered scattered laser radiation; and 4) filtered
backscattered laser radiation or filtered scattered laser
radiation.
[0079] After detecting the four components of laser radiation, a
computer (e.g., computer 156, FIG. 2), determines normalized filter
transmission of the vapor filter, in step 403. For example, the
computer, in one embodiment, processes the unfiltered laser
radiation and filtered laser radiation by dividing the magnitude of
the filtered laser radiation by the magnitude of the unfiltered
laser radiation. In one embodiment, the division is performed on a
pulse-by-pulse basis, where divided magnitudes of the pulses have
corresponding frequencies.
[0080] The computer also determines, in one embodiment, a
normalized atmospheric return of the laser radiation, in step 404.
For example, the computer may process the filtered backscattered
laser radiation and unfiltered backscattered laser radiation by
dividing the magnitude of the filtered backscattered laser
radiation by the magnitude of the unfiltered backscattered laser
radiation. Again, in one embodiment, division is performed on a
pulse-by-pulse basis, where divided magnitudes of the pulses have
corresponding frequencies.
[0081] Once normalized filter transmission and normalized
atmospheric return of the laser radiation are determined, the
computer determines signal strengths for each of the filter
transmission and the atmospheric return. For example, the computer
determines the optical transmission through the filter by
calculating a ratio of the filtered laser radiation to the
unfiltered laser radiation at particular frequency ranges, in steps
405 and 407. The computer similarly determines the atmospheric
return (scattering) signal strength through the filter by
calculating a ratio of the filtered backscattered laser radiation
to the unfiltered laser radiation at particular frequency ranges,
in steps 406 and 408.
[0082] The computer also determines a signal strength ratio for the
normalized filter transmission by dividing filtered laser radiation
by unfiltered laser radiation, again on a pulse-by-pulse basis, at
frequencies greater in magnitude than about +/-18 GHz about the
peak absorption frequency, in step 407. The computer further
determines a signal strength ratio for the normalized filter
transmission by dividing filtered laser radiation by unfiltered
laser radiation on a pulse-by-pulse basis at frequencies between
about +/-0.5 GHz, in step 405. These signal strength determinations
correspond to frequency ranges where Mie scattering (e.g., +/-18
GHz) and Rayleigh scattering (e.g., +/-0.5 GHz) are most prevalent,
and are thus useful when combined with similar signal strength
determinations for the normalized atmospheric return. The computer
determines a Mie scattering signal strength ratio for the
normalized atmospheric return of the laser radiation by dividing
filtered backscattered laser radiation by unfiltered backscattered
laser radiation, again on a pulse by pulse basis, at frequencies
greater in magnitude than about +/-18 GHz about the peak absorption
frequency, in step 408. The computer also determines a Rayleigh
scattering signal strength ratio for the normalized atmospheric
return of the laser radiation by dividing filtered scattered laser
radiation by unfiltered backscattered laser radiation on a
pulse-by-pulse basis at frequencies between about +/-0.5 GHz in
step 406.
[0083] With signal optical transmission for the filter and signal
strengths for both Rayleigh scattering and Mie scattering
determined, the computer determines a Rayleigh laser filter
convolution in step 409. For example, the computer, in one
embodiment, performs a convolution of the optical transmission with
the Rayleigh and Mie scattering signal strengths corresponding to
the frequency ranges for Rayleigh and Mie scattering of +/-0.5 GHz
and +/-18 GHz, respectively. The computer then accesses a lookup
table, such as lookup table 170 of FIG. 2, that has theoretical
Rayleigh laser filter convolution values to determine temperature
and pressure of the air, in step 410.
[0084] It is also possible to calculate a convolution of a measured
filter function with a theoretical Rayleigh-Brillouin return
(Rayleigh line shape), and directly compare the convolution with
filtered scattered laser radiation. This allows calculation of
atmospheric parameters without calculating a deconvolution of the
Rayleigh-Brillouin signal, reducing the complexity of real-time
calculations required to determine the atmospheric parameters. In
particular, ratios of measured signals may be compared directly to
theoretical ratios of a Rayleigh line shape convolved with measured
filter functions to allow self calibrating measurements. For
example, signal strength variations across data gathering channels
and power of scattered laser radiation may be inherently normalized
when such ratios are used. Certain ratios of measured data at laser
frequencies that lie within filtered bands of optical notch filters
(e.g., absorption features of an atomic vapor cell, or equivalent
features of other filters, as discussed above) may be useful for
determining temperature and pressure, since Mie scattering is
eliminated firm the measured data. Calculation of convolutions may
represent a lower computational burden on a computer (e.g.,
computer 156 of OADS 140) as compared to calculating deconvolutions
of measured data into and out of a Rayleigh-Brillouin
representation.
[0085] For example, filtered scattered laser radiation data in a
signal channel may characterized by the equation:
S S ( v ) = P L T L T R E S D S .intg. .intg. v 1 v r L ( v laser )
F ( v 1 - v ) ( rR ( v - ( v r - .DELTA. v D ) ) + mM ( v - ( v r -
.DELTA. v D ) ) ) ( Eq . 24 ) ##EQU00019##
where parameters are as previously defined, and a subscript 1
indicates a measurement frequency 1. Eq. 24 may be simplified by
using the notation LFR(.nu.) for the convolution of laser, filter
function and Rayleigh return, as defined above, and a similar
notation LFM(.nu.) for a convolution of laser, filter function, and
Mie scattering return:
S S ( v 1 ) = P L I T L I T R I E SI D SI [ r L F R ( v 1 ) + m L F
M ( v 1 ) ] ( Eq . 25 ) ##EQU00020##
[0086] If frequency 1 is located in a filter absorption band, the
Mie scattering term is effectively eliminated, yielding:
S.sub.S(.nu..sub.1)=P.sub.LIT.sub.LIT.sub.R1E.sub.S1D.sub.S1rLFR(.nu..su-
b.1) (Eq. 26)
Forming a ratio of a signal obtained at frequency 1 with a signal
obtained at another frequency 2 in another filter absorption band
yields:
S S ( v 1 ) S S ( v 2 ) = [ P La L La T Ra E Sa D Sa P Lb L Lb T Rb
E Sb D Sb ] [ r a ( r b + m b ) r b ( r a + m a ) ] [ LFR ( v 1 )
LFR ( v 2 ) ] ( Eq . 27 ) ##EQU00021##
where frequency 1 is measured at time a and frequency 2 is measured
at time b. If times a and b are close enough to each other that no
atmospheric changes occur between time a and time b (or if
measurements are interspersed in such a way that average values of
parameters such as P, L, T, E, D and r are identical over a time
span of the measurements) then the ratio of Eq. 27 simplifies
further to:
S S ( v 1 ) S S ( v 2 ) = LFR ( v 1 ) LFR ( v 2 ) ( Eq . 28 )
##EQU00022##
[0087] In one embodiment, a lookup table stores temperature and
pressure pairs that correspond with two of the measurement ratios
defined in Eq. 28. The two ratios essentially define two equations
with two unknowns (i.e., a single such ratio may not determine both
pressure and temperature). Data may also be taken in more than
three filtered bands, yielding more than two of the Eq. 28 ratios;
when more than two such ratios are available, multiple values of
temperature and pressure may be determined that may be averaged or
used in "best fit" methods to improve temperature and pressure
determination in a noisy measurement environment.
[0088] In an embodiment, theoretical Rayleigh line shapes
corresponding to temperature and pressure combinations are stored
in a lookup table. A reference curve is calculated by obtaining a
Rayleigh line shape corresponding to an estimated temperature and
pressure from the lookup table and convolving the Rayleigh line
shape with a normalized atmospheric return curve. Values of
LFR(.nu.) at absorption feature maxima may then be determined from
the reference curve and used to determine one or more air
parameters (e.g. temperature and/or pressure) using Eq. 28.
[0089] Calculating convolution of the measured filter function with
the theoretical Rayleigh line shape also enables utilization of
curve fitting routines to map the convolved curves to true
temperature and pressure conditions, such that the deconvolution
calculations suggested by the Tenti, Boley and Desai paper above
are not required. An OADS may store a pre-compiled table of stored
curve shapes that are generated by modeling large databases of
known temperature and pressure values (e.g., the table may be
stored in computer 156 of OADS 140). As measurements are taken,
data curves may be generated from measured data, and curve-fitting
routines may be used to compare the data curves to the stored curve
shapes to derive true temperature and pressure. The utilization of
curve-fitting routines may also have less sensitivity to noisy
data, as compared to deconvolution calculations, making the
determination of true temperature and pressure more robust.
[0090] FIG. 9 is a flowchart showing one exemplary method of
operation 450 of an OADS, which may be used to calculate one or
more air parameters. Method 450 may be partially or fully performed
by computer 156 of OADS 140; computer 156 may receive operating
instructions from software and/or firmware.
[0091] In an embodiment of step 460, a laser (e.g., laser 141 of
FIG. 2) sweeps laser radiation across a predetermined frequency
range (swept frequency range) that is centered about a deep
absorption line of a filter. The laser may sweep the laser
radiation across a swept frequency range of about +/-20 GHz by
transmitting the laser radiation at a certain PRF, or by sweeping
the frequency of a continuous wave laser. In one embodiment, a PRF
is about 1 kHz, with a pulse width between about 50 ns and 100 ns,
and the swept frequency range is centered about a frequency
corresponding to a peak absorption frequency (e.g., 260 nm) of a
filter (e.g., vapor filter 152, FIG. 2, or an interference filter,
a fiber Bragg grating filter, a dichroic filter, a volume
holographic grating filter, or a Rugate filter). In an embodiment,
the swept frequency range includes frequencies corresponding to at
least two absorption features of at least one band stop filter. In
another embodiment, the swept frequency range includes frequencies
corresponding to at least three absorption features of at least one
band stop filter.
[0092] Step 462 detects laser radiation corresponding to filtered
scattered laser radiation (e.g. component 157 of FIG. 2), filtered
laser radiation (e.g. component 164 of FIG. 2), and unfiltered
laser radiation (e.g. component 159 of FIG. 2) at each frequency;
each step 460 and 462 is for example performed for each laser pulse
in the swept frequency range.
[0093] Step 464 determines a normalized filter transmission curve
by dividing a magnitude of filtered laser radiation by a magnitude
of unfiltered laser radiation for each pulse in the swept frequency
range; step 466 determines a normalized atmospheric return curve by
dividing a magnitude of filtered scattered laser radiation by a
magnitude of unfiltered laser radiation for each pulse in the swept
frequency range. It will be appreciated that since the data
required for the calculations in steps 464 and 466 are collected by
the operation of steps 460 and 462, steps 464 and 466 may be done
in any order or in parallel.
[0094] Step 468 calculates a Doppler shift .DELTA..nu..sub.D that
is a frequency shift between the normalized filter transmission
curve (calculated in step 464) and the normalized atmospheric
return curve (calculated in step 466), then calculates a local
radial wind velocity V.sub.R using Eq. 1 above. As was stated
above, a band stop filter may have a plurality of absorption
features; consequently, a plurality of Doppler shift
.DELTA..nu..sub.D and radial wind velocity .nu..sub.R calculations
may be calculated in step 468.
[0095] Step 470 utilizes only normalized atmospheric return curve
magnitude values (calculated in step 466) within three or more
specific filter absorption bands to form two or more normalized
atmospheric return ratios (actual ratios). For example, if
atmospheric return data is derived for frequencies 1, 2, and 3 (at
times that are close enough together, as discussed with reference
to Eq. 28 above), then two ratios may be formed using one of the
frequencies as a baseline (denominator), such as
S S ( v 1 ) S S ( v 2 ) and S S ( v 3 ) S S ( v 2 ) .
##EQU00023##
Atmospheric return curve magnitude values corresponding to
absorption feature maxima of one or more band stop filters may be
used. One atmospheric return ratio (actual ratio) may be determined
if for example only one air parameter (e.g. pressure or
temperature) is to be calculated.
[0096] Step 472 obtains theoretical temperature and pressure data
from a lookup table of normalized filter transmission convolved
with theoretically derived Rayleigh line shapes, at the frequencies
utilized in step 470. One or more air parameters (e.g. temperature
and/or pressure) are then estimated. A Rayleigh line shape
corresponding to the estimated one or more air parameters is for
example obtained from a lookup table. A reference curve is then
calculated by convolving the Rayleigh line shape with the
normalized filter transmission curve from step 464.
[0097] In step 474, ratios corresponding to the ratios formed in
step 470 are formed from magnitude values of the reference curve
calculated in step 472. The ratios formed in step 474 may be
referred to as reference ratios.
[0098] In step 476, one or more air parameters (e.g. temperature
and pressure) are determined. An error corresponding to the
differences between the one or more actual ratios and the
corresponding one or more reference ratios may be calculated: if
the error is within an acceptable range, the estimated one or more
air parameters (corresponding to the Rayleigh line shape) are
published as the actual one or more air parameters; but if the
error is not within an acceptable range, steps 472, 474, and 476
are repeated with one or more different estimated air parameters
until the error is within an acceptable range.
[0099] The error of step 476 may be calculated using a least mean
square error algorithm. Steps 470, 474, and 476 may be optional;
the normalized atmospheric return curve calculated in step 466 is
for example correlated to the reference curve calculated in step
472 using curve fitting routines.
[0100] Certain advantages of embodiments described above may
include: [0101] (1) Obtaining accurate computations of various air
parameters, such as air speed, air temperature and air pressure,
substantially regardless of altitude and/or Mie scattering; [0102]
(2) Obtaining a system that accurately performs in a variety of
vibrational environments; [0103] (3) Obtaining an ability to
determine temperature and pressure within a particular region of
atmosphere without a prior knowledge of the atmosphere; [0104] (4)
Reducing need for on-aircraft system calibrations and system health
checks, as compared to existing systems; [0105] (5) Providing
robustness with respect to high vibration environments; [0106] (6)
Obtaining faster calculations and/or reduced computational
requirements placed on aircraft computers, as compared to existing
systems; [0107] (7) Ability to accurately calculate velocity in
environments with changing temperature and/or pressure; and/or
[0108] (8) Ability to accurately calculate one or more air
parameters (e.g. velocity, temperature, and/or pressure) without
precise control of laser frequency.
[0109] It can be desirable to measure air parameter, such as
velocity and temperature, at selected distances (or ranges) from an
Outside Air Data System. In an aircraft, discrepancies between air
velocity near the aircraft and air velocity in a more distant zone
ahead of the aircraft can provide warning of wind shear or
microburst activity. In ground-based applications, it is known that
wind speed, wind direction, and air temperature can vary with
altitude, and altitude above an air data system corresponds to
range above the system.
[0110] An OADS of the type discussed herein with reference to FIGS.
1-9 can be operated in a pulsed mode. In this mode, each time laser
141 emits a pulse of laser radiation, measurements are taken by
detector 153 at one or more of several specific time delays
following the pulse. Air data parameters derived from measurements
made at each specific time delay from the pulse correspond to air
data parameters at a particular distance or range from the OADS
system.
[0111] An alternative embodiment of the OADS that provides for
range resolution and permits use of lower cost lasers by allowing
the OADS to operate at a lower peak laser output power is the
"Random Modulated Continuous Wave" (RMCW) approach illustrated in
FIG. 10. In this system, a pseudorandom sequence generator 550
generates continuously, and repeatedly, a binary pseudorandom code
sequence. The pseudorandom code possesses a delta-function
autocorrelation, meaning that a mathematical cross-correlation of
the code with itself produces a delta function at zero time delay.
The pseudorandom code is sent to an amplitude modulator 553, which
amplitude-modulates a tunable laser 552; tunable laser 552
corresponds to laser 141 of FIG. 2. Modulator 553 may be an
integral subsection of the laser 552, such is the case with diode
lasers, or may be separate component exterior to laser 552, such as
Lithium:Niobate modulators, acousto-optic modulators or similar
devices. Laser radiation from laser 552 enters a beam splitter 554.
A portion of radiation from beam splitter 554 passes through filter
556 and reaches detector 558. Another portion of radiation from
beam splitter 554 is transmitted into the air, is scattered by, and
subjected to Doppler shift by, aerosol and molecular scatterers
560, and returned to the OADS where it passes through filter 556 to
detector 562.
[0112] Meanwhile, the pseudorandom code from sequence generator 550
is passed to a digital signal processor 554 to be used in
interpreting the output from detector 562. The output from detector
562 is first converted to a digital representation using the
analog-to-digital converter 563. For each of the pseudorandom code
generated by sequence generator 550, the output from the
analog-to-digital converter 563 is added into a unique memory
location. These "n" unique memory locations are collectively termed
a Histogramming Memory 555. Likewise, the Histogramming Memory 555
returns to the first unique memory location and begins summing each
new output from the analog-to-digital converter 563 to accumulated
value contained in each unique memory location, starting with the
first unique location and proceeding in sequence. This continuous
process is repeated once, or as many times as desired.
[0113] One embodiment repeatedly transmits and collects sufficient
iterations through the pseudorandom sequence into the Histogramming
Memory 555 until a sufficient lidar Signal-to-Noise Ratio (or
similar lidar system performance metric) is achieved. Once
sufficient data is collected in the Histogramming memory 555, the
"n" values accumulated into the "n" unique memory locations are
passed to the digital signal processor 554. The digital signal
processor 554 performs a mathematical cross-correlation on the two
"n" valued sequences: one arriving from the pseudorandom code
generator 550 and one arriving from the Histogramming Memory 555.
The resultant output is termed the correlated signal 570 and
provides the range-resolved return signal. The correlated signal
570 is then used to determine air parameters at all specific
distances from the OADS.
[0114] During hot summer days in large parts of the United States,
air 604 is heated near the surface, as for example a runway 602
(FIG. 11). By afternoon, this often results in "unstable air"
conditions, where warm air 604 may rise 606, sometimes rapidly. Air
is drawn inward towards the base of the resultant rising column of
air, and may begin to rotate. Depending on conditions, the
resultant disturbance may range from a "dust-devil" to trigger more
widespread phenomena like a thunderstorm, hurricane, or tornado.
Even a dust-devil can pose hazard to an aircraft that attempts to
land or takeoff through it. Similarly, dust-devils can cause sharp
wind gusts that can pose problems for wind power systems they may
encounter.
[0115] Rising hot air may carry moisture with it, and may rise to
high altitudes where the moisture condenses into rain. Falling rain
may drag an air column downwards 608, sometimes quite quickly.
Since the ground impedes airflow, air from the down-moving air
column 608 may blast outwards in one or more directions from a
center of the column in a phenomenon known as a microburst.
Aircraft typically land along a glideslope 610 of between three and
six degrees from the horizontal, and typically maintain a
predetermined approach airspeed along an approach path aligned with
the runway while doing so. According to investigators, a Lockheed
L-1011 attempted landing at Dallas while a microburst intersected
the approach path. As it descended along the glideslope, it first
met with headwinds, then a downdraft, and finally a tailwind. The
L-1011 slowed to maintain airspeed while in the headwind, and by
the time it passed through the downdraft into the tailwind zone it
had insufficient airspeed to continue flying--and sank into the
ground short of the runway. This accident led to great interest in
detecting microbursts and other low-level wind shear near airports
so that similar events can be avoided.
[0116] Wind power systems, such as illustrated in FIG. 12, produce
power in amounts that vary drastically with wind velocity. In
particular, no power is generated when wind velocity falls below a
minimum, or cut-in, windspeed, this minimum is a function of
specific wind turbine parameters including gear ratio between hub
and generator, generator design, blade design, and blade length.
These wind turbine parameters also partly determine an optimum
power generating wind velocity range for the wind turbine.
[0117] Wind power systems may also be damaged by high winds or
turbulence, wind turbines typically have maximum allowable wind
conditions for operation determined by these wind turbine
parameters as well as other wind-turbine specific parameters such
as tower height and strength, blade strength, and hub bearing
design--when wind velocity or turbulence exceeds this maximum the
wind turbine generally must furl and when furled generates no
power. Since wind may vary with season, as well as with terrain, it
is desirable to record wind conditions at brief intervals over an
extended time--extending over at least several months to a year--to
determine suitable locations and optimum wind-turbine
specifications for construction of wind power systems or
wind-farms. It is desirable to obtain wind speed and direction data
at multiple altitudes at each proposed site, including at the
surface, at hub altitude, and at blade minimum and maximum
altitudes; obtaining this data is part of a site survey for a wind
power system. The accumulated data may be used to determine optimum
wind-turbine specifications for, and predict expected power output
of the wind-power system from, a wind power system or wind
farm.
[0118] Typically, wind power systems have an array of one or more
wind turbines 702. Large wind power systems, known as wind farms,
may include dozens or even hundreds of individual wind turbines
near each other and located in favorable locations having favorable
wind, such as the Altamont Pass near Livermore, Calif. Each wind
turbine 702 of the system has one, two, or more blades 704 attached
to a hub 706 that directly, or indirectly through a transmission,
drives a generator that is typically located in a nacelle 708.
[0119] Most wind turbines are of the horizontal axis type, and
require an orientation subsystem to ensure the wind turbine and its
blades are maintained at a proper angle to the wind despite changes
in wind direction. The orientation subsystem may take the form of a
tail 710 as commonly used with smaller wind turbines having blades
upwind of tower 712. In some other wind turbines 713, the
orientation system has a pivot (not shown) under the nacelle 715
with blades 717 placed on a downwind side of tower 712 such that
wind drag on the blades tends to orient the wind turbine at a
correct angle to the wind. The orientation subsystem typically
includes a pivotable attachment (not shown) of nacelle 708, 715 to
tower 712. Other forms of active and passive orientation systems
are known.
[0120] Many wind turbines have a furling system which coarsens or
feathers blade pitch, or directs the blades away from the wind, to
protect the turbine from potentially damaging winds such as wind
gusts or high winds and storm conditions; the furling system may
interact with the orientation system or with a blade pitch system,
other variations are known including air brakes, mechanical brakes,
and retractable mountings.
[0121] Many wind turbines have a pitch system for controlling blade
pitch, where an angle of attack of blade 704 to wind is varied from
a fine pitch in low winds through a coarse pitch in higher winds to
a feathered pitch in potentially damaging wind conditions--blade
pitch control can serve as a furling system. Some larger wind
turbines have independent blade pitch control where the angle of
attack of the blades can be adjusted independently, and in some
systems blade pitches can be independently adjusted cyclically
through a revolution.
[0122] Electrical energy is collected from generators of all wind
turbines 702 of a system by energy collection and processing
apparatus 720; once collected the energy may be fed to the power
grid, stored for later use, or used locally.
[0123] Wind turbines are available in a wide variety of types and
sizes ranging from small turbines of a few watts capacity, such as
have been used to provide a small amount of electrical power to a
glider or airplane, through turbines of a few hundred or a few
thousand watts capacity such as are often used for off-grid
residences, to large turbines having over 2 megawatts of peak
output capacity and which typically feed a large power grid. Wind
systems may include more than one type of wind turbine, and may be
supplemented or collocated with other types of renewable and/or
non-renewable energy generation apparatus.
[0124] Wind turbines 702 and associated towers 712, including
blades 704, are subject to variable, and occasionally large, wind
loads. Since blades 704 are often quite long, their rapidly
rotating mass combined with high and possibly imbalanced wind loads
can cause substantial vibration and stress at nacelle and tower.
Excess wind loads have caused damage to turbines and towers, up to
and including collapse.
[0125] Wind shear is a local weather condition where wind velocity
and/or direction varies with altitude, this can result from
turbulence from hills, trees, other wind turbines, and ridgelines
as well as from convective phenomena like microbursts and
dust-devils. In addition to wind shear posing a hazard to aircraft
near an airport, it also poses a hazard to wind turbines as blades
may be exposed to wind forces that vary substantially through a
revolution, in turn aggravating vibration and load stress. A
standard solution to this problem is to increase tower height so
that the wind turbine is exposed to more uniform wind than
available at lower altitude--this can greatly increase tower
expense and strength requirements and other solutions are
desirable. Vibration over extended periods has caused damage to
turbines and towers, including metal fatigue of towers. If wind
speed and direction versus altitude are known, vibration induced by
wind shear can also be reduced by adjusting blade pitch as a blade
swings from one altitude to another, such that stress on high
blades is more evenly balanced by stress on lower blades.
[0126] It is known that thunderstorms, microburst, and dust-devil
conditions, as well as other weather conditions, can cause gusty
conditions that may result in a wind load on a blade 704 of a wind
turbine changing dramatically in a matter of seconds; these
conditions can therefore change from good power-generation
conditions to conditions requiring altered blade pitch or even
rapid furling to avoid excessive wind load and damage to the
turbine or tower.
[0127] Many wind turbines sense changed wind conditions by
monitoring power output and/or rotational rate of blades 704, these
wind turbines can only respond alter changes have occurred.
[0128] A ground-mounted air data system 714 may be located near one
or more wind turbines of a system to provide additional and early
real-time wind information, and information regarding unstable air
conditions, with which to optimize blade pitch, or to furl, before
those conditions reach the wind turbine. Similarly, an air-data
system 722 may be located in a hub or nacelle of a wind turbine to
provide information on approaching winds--including warning of
oncoming gusts.
[0129] U.S. Pat. Nos. 7,342,323, 7,281,891, and 6,320,272 describe
wind turbines that include laser wind velocity measurement systems
mounted on the nacelle or on a hub of a wind turbine, to determine
the air velocities in front of the wind turbine. The systems change
blade pitch dependent on measured on-coming wind velocities. All of
these systems use a coherent, pulsed or continuous wave, lidar.
Such systems can only use Mie scattering and cannot utilize
Rayleigh scattering, decreasing their measurement robustness in
clear atmospheric air and precluding their ability to measure
atmospheric temperature or pressure. Such systems measure
velocities but assume that wind direction is constant with altitude
and aligned with the wind turbine's axis. Some of these systems
measure windspeed variation with altitude; the system of 7,281,891
in particular has an off-axis hub-mounted lidar that scans a
conical region ahead of the turbine as the turbine rotates. The
system of 7,281,891 discloses detection of windspeed by Doppler
lidar techniques over a conical scanned region, but does not
disclose detection of temperature or details of lidar operation and
range determination.
[0130] We therefore offer a ground-based wind mapping system for
site survey and/or system control that is capable of mapping and
recording wind direction and velocity, along with air temperature,
at a variety of altitudes and ranges of interest to a wind power
system, even when the atmosphere is very clean of aerosols. We also
offer a hub mounted system capable of mapping wind direction and
velocity at a range of altitudes and ranges in a zone upwind of a
wind turbine.
[0131] A ground-based air-data system 800 may be assembled as shown
in FIG. 13 by assembling three laser transceivers 802, 804, 806
such as the Rayleigh-Mie transceiver device previously described
with reference to FIGS. 1-10 into a common housing 808 and a window
810. All three transceivers provide data to, and operate under
control of, computer 812. All three transceivers 802, 804, 806 are
aimed through the common window 810, however each is aimed along a
slightly different axis 814, 816, 818, such that the three axes do
not lie in a common plane.
[0132] Computer 812 uses each of transceivers 802, 804, 806 to
measure a Doppler-shift at a first distance from the system 800.
These Doppler-shifts are used, together with a known orientation of
the system, by computer 812 to compute a windspeed and direction at
that distance or altitude. Similarly, computer 812 uses at least
one of transceivers 802, 804, 806, to sense temperature at the same
altitude. In an embodiment, windspeed, wind direction, and air
temperature are sensed and recorded at several altitudes ranging
from zero to two thousand feet, or higher, at periodic time
intervals.
[0133] The embodiment of FIG. 13 may be combined with a solar power
system 830 and digital data recorder 832 to perform site monitoring
of a proposed location for wind power systems, in an embodiment the
digital data recorder 832 records minimum, average, and peak-gust
windspeed with air temperature at four selected altitudes at
fifteen minute intervals, and has storage capacity sufficient to do
so for at least a month without overwriting recorded data. Other
embodiments may record additional data, an anticipated embodiment
records minimum, average, and maximum wind speed and direction
observations from six altitudes at ten minute intervals. Yet other
embodiments of the site survey system may include scanning of an
area, as described below with reference to the embodiment of FIG.
15, and recording of windspeed and direction data at multiple
altitudes at multiple locations in an area of interest.
[0134] The embodiment of FIG. 13 may also be located at an airport
to sense wind shear and other wind hazard conditions. Likewise, the
embodiment of FIG. 13 may also be used to monitor wind speed and
temperature profiles for meteorological applications, including
weather monitoring and prediction.
[0135] Similarly, embodiments of FIG. 13 may be placed at an
airport and aligned along an approach path and glideslope. Since
aircraft will be flying towards them, it is necessary that these
systems use long wavelengths such as 1500 nanometers that are
invisible and non-harmful to the human eye. These devices measure
windspeed and direction at several distances along the glideslope;
this data can be processed to provide warnings of convective
instability, low level wind shear, dust-devil, tornado, hazardous
crosswinds, microbursts and similar wind-related hazardous
conditions.
[0136] In an alternative embodiment of the ground-based air-data
system 900, as illustrated in FIG. 14, a transmitter assembly 902
is adapted to provide pseudorandom modulation from modulator 903 to
three (or more) incoherent RMCW transmitter laser-telescope
transmitter assemblies 904, 906, 908. Each of the three (or more)
transmitter laser-telescope assemblies 904, 906, 908 are aligned on
a different axis 910, 912, 914, the axes oriented such that the
three axes are not mutually coplanar, and aimed through window 916
in a housing 918. Each of the transmitter laser-telescope
assemblies transmits modulated laser radiation into the air along
its associated axis, where Mie and Rayleigh scattering will take
place. In a particular embodiment, the transmitter laser-telescope
assemblies operate at 1550 nanometers.
[0137] Similarly, a receiver assembly 920 has three (or more)
photodetector-telescope assemblies 922, 924, 926 each aligned on an
axis 928, 930, 932. Each of these receiver axes 928, 930, 932 is
aligned parallel to, and slightly converging with, a transmitter
axis 910, 912, 914. Receiver electronics 940, 942, 944 receives
signals from an associated photodetector-telescope assembly 922,
924, 926 and correlates the received signal with modulation as
sampled from the modulator 903 to provide distance-resolved
measurements of Doppler shift of Mie and Rayleigh-scattered
radiation received by the associated photodetector-telescope
assembly.
[0138] Computer 950 receives information from all three (or more)
receiver electronics 940, 942, 944 and calculates windspeed and
wind direction at various ranges from the apparatus 900 from the
received Rayleigh and Mie-scattering data; updating detected
windspeed and wind direction measurements every tenth of a second,
or faster, as required.
[0139] In a particular embodiment, one of the transceivers 904/926,
or an additional laser transceiver 952 as previously described with
reference to FIGS. 1-10, is used to determine temperature at
various ranges from the unit. This unit therefore can provide a
profile of windspeed, direction, and temperature with altitude,
these measurements can be compared to limits to provide warning of
wind-shear at airports or recorded with a digital recorder to
perform site survey for wind power systems. Further, with the aid
of a separate ground-level humidity sensor, temperature versus
altitude data from the system is processed to provide a measure of
convective instability; this measure of convective instability
provides an early warning of conditions when convective activity
such as dust-devils, microbursts, thunderstorms, and tornadoes are
likely to develop even if such wind conditions do not yet exist in
the field of view of the system.
[0140] Temperature versus altitude measurements may be combined
with a humidity measurement from other apparatus to give a measure
of instability of air. Since unstable air can lead to and powers
convective activity, ranging from simple dust-devils to tornadoes
all of which may produce gusty conditions; furling thresholds may
be reduced by a wind turbine controller when unstable air
conditions exist.
[0141] An alternative embodiment of the OADS 1000 is illustrated in
FIG. 15. In this embodiment, at least one air data laser
transmitter, 1002, and receiver, 1004, as previously discussed with
reference to the RMCW OADS of FIGS. 1-10, are aimed at a scanning
wedge, 1006, or a holographic grating or steering mirror, for
example, that sweeps out an area of interest. The scanning wedge
redirects its field of view. The scanning wedge 1006 is attached to
a motorized mount 1008 that moves the wedge to scan the field of
view of the air data laser transmitter and receiver 1002, 1004
vertically so that field of view is scanned over a range of angles
such as angles ranging from the horizon to directly above the
OADS.
[0142] In an embodiment, the air data laser transmitter 1002,
receiver 1004, mirror 1006, and motorized mount 1008 are mounted
within a rotatable turret 1010, rotatable turret 1010 is arranged
such that the field of view of the OADS is scanned horizontally
over a 360-degree region around the OADS. In an alternative
embodiment, the laser transmitter 1002 and receiver 1004 are
stationary, but scanning wedge 1006 is rotated by motorized mount
1008 to scan. In this way, the field of view of the OADS is scanned
over a hemispherical volume of air centered on the location of the
OADS and of radius up to two or more kilometers.
[0143] An additional embodiment the OADS resembling that of FIG. 15
includes one air data laser transmitter, 1002, and receiver, 1004,
as previously discussed with reference to the RMCW OADS of FIGS.
1-10, is aimed at dual prisms or holographic gratings, (not shown)
to direct the scan to any predetermined point in a conical field of
view.
[0144] An embodiment of the OADS of FIG. 15 has three laser
transceivers 1002, 1004 and uses Doppler measurements of all three,
with RMCW range discrimination, to determine windspeed and wind
direction at various regions of interest in the hemispherical
volume of air.
[0145] An alternative embodiment of the OADS of FIG. 15 obtains the
three Doppler measurements required for wind direction measurements
in a region of the hemispherical volume of air from a single laser
transmitter 1002 and receiver 1004 by recording Doppler shift
measured at two slightly-different vertical angles and two
slightly-different horizontal turret or scanning wedge angles. This
embodiment is also capable of mapping windspeed and wind direction
throughout the hemispherical volume of air.
[0146] The OADS of FIG. 15 may be located 714 (FIG. 12) near a wind
turbine 702, or near a group of wind turbines, to provide air data
at a variety of positions and altitudes for control of the turbines
702. This OADS is capable of detecting wind shear and adverse wind
conditions, and adjusting wind turbine 702 by adjusting blade pitch
cyclically during turbine rotation, in some embodiments trimming
yaw through adjustment of an active orientation subsystem, and
furling when necessary, to reduce loads incurred by the blades 704;
thereby enabling the wind turbine 702 to better survive. In an
embodiment, the wind turbine is therefore better able to survive
turbulence and wind shear having differences in wind direction as
well as wind speed with altitude and enabled to provide power in
conditions that may otherwise require furling. The system therefore
provides better protection and utility of wind turbines than
systems known in the art. In an embodiment, the computer of the
RMCW OADS is programmed to ignore scatter from angles and delays,
and hence locations, coincident with locations of wind turbines to
avoid reading blade motions as wind.
[0147] In another embodiment the RMCW OADS of FIG. 15 may be
mounted on the nacelle 708 of a wind turbine and programmed to
ignore scatter from angles and delays, and hence locations,
coincident with the blades of the wind turbine. In an embodiment,
the computer of the RMCW OADS is programmed to ignore scatter from
locations of other wind turbines of the wind farm to avoid reading
blade motions as wind.
[0148] Similarly, the OADS of FIG. 15 may be located near a runway
for mapping wind near an airport, or may be positioned at a
proposed wind-farm site for site survey purposes.
[0149] Similarly, the OADS of FIG. 15 may be located in an area,
such as a mountain pass, where high, gusty, or turbulent winds may
reach levels that pose danger to trucks and other high profile
vehicles. The computer of this OADS is programmed to generate
traffic alerts when high, gusty, or turbulent winds exceeding a
predetermined threshold are detected.
[0150] In an alternative embodiment, an RMCW OADS as described with
reference to FIGS. 1-10 or FIG. 13 is located 722 in a hub 704 of a
wind turbine 702. This OADS is mounted with an axis off-axis with
respect to an axis of the wind turbine, such that it maps windspeed
and direction at several ranges of a cone 724 ahead of the wind
turbine 702. The computer of the RMCW OADS is programmed to ignore
scatter from angles and ranges coincident with locations of other
wind turbines of the wind farm to prevent reading blade motion as
wind.
[0151] Since this OADS can sense wind direction, and wind direction
variation with range and altitude, as well as wind speed, it
detects direction as well as velocity components of wind shear. The
OADS therefore provides information for wind turbine 702 to furl or
otherwise compensate for such wind shear.
[0152] In an alternative embodiment (not illustrated), the OADS is
mounted in a blade of a wind power system, and provides both
angle-of-attack and relative speed information of wind to blade.
This information is used to control blade pitch. The information
may also be stored at multiple points during a rotation and used to
adjust blade pitch through each rotation of the blade.
[0153] Since certain changes may be made in the above methods and
systems without departing from the scope of the disclosure herein,
it is intended that all matter contained in the above description
or shown in the accompanying drawings be interpreted as
illustrative and not in a limiting sense. By way of example, those
skilled in the art should appreciate that the OADS and the OADS
transceivers, as described herein, may be constructed, connected,
arranged, and/or combined in ways that are equivalent to what is
shown.
* * * * *